Causal characteristic impedance determination using calibration comparison and propagation constant

S Amakawa, A Takeshige, S Hara… - 2019 92nd ARFTG …, 2019 - ieeexplore.ieee.org
S Amakawa, A Takeshige, S Hara, R Dong, S Lee, T Yoshida, M Fujishima, K Masu, H Ito
2019 92nd ARFTG Microwave Measurement Conference (ARFTG), 2019ieeexplore.ieee.org
It is common to determine the characteristic impedance Z_0 of a low-loss transmission line
using the measured propagation constant γ through Z_0=γ/(G+jωC), assuming that the
parallel conductance G=0 and that the parallel capacitance C is constant. However, if the
line is a coplanar waveguide or a microstrip, two dielectrics (substrate and air) are involved
and its effective dielectric constant is frequency-dependent, which makes C also frequency-
dependent. If so, the assumption G=0 is inconsistent with causality constraints. This paper …
It is common to determine the characteristic impedance of a low-loss transmission line using the measured propagation constant through , assuming that the parallel conductance and that the parallel capacitance is constant. However, if the line is a coplanar waveguide or a microstrip, two dielectrics (substrate and air) are involved and its effective dielectric constant is frequency-dependent, which makes also frequency-dependent. If so, the assumption is inconsistent with causality constraints. This paper presents an attempt at determining by augmenting the above method in a way consistent with causality. A method of calibration comparison with 2nd-tier multiline TRL is used to extract and , following 1st-tier probe-tip calibration that is assumed to be valid at least up to 67 GHz. Then, a causal model, , of parallel admittance is built from GHz) by network synthesis. and are then used to determine including GHz. The method is applied to a CMOS transmission line from 20 MHz to 220 GHz. A well-built model gives well-behaved and plausible estimate of causal over the entire measurement frequency range.
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